Physics 101: Lecture 12, Pg 1 Physics 101: Lecture 12 Collisions and Explosions l Today’s lecture covers Textbook Sections 7.5 - 7.8 Exam II.

Slides:



Advertisements
Similar presentations
Chapter 7 Collisions. If the sum of the external forces is zero, then PRINCIPLE OF CONSERVATION OF LINEAR MOMENTUM The total linear momentum of an isolated.
Advertisements

Physics 111: Lecture 14, Pg 1 Physics 111: Lecture 14 Today’s Agenda l Momentum Conservation l Inelastic collisions in one dimension l Inelastic collisions.
Physics 101: Lecture 13 Rotational Kinetic Energy and Inertia
SPH4U Agenda Impulse Collisions: you gotta conserve momentum!
Linear Momentum and Second Newton’s Law Definition of momentum: Change in momentum: 2 nd Newton’s Law: Definition of acceleration: We can write 2 nd Newton’s.
Momentum and Collisions
Classical Mechanics Lecture 11
1 Chapter Six: Momentum and Collisions. 2 Momentum is the product of the mass of a body and its velocity. A body may be an assembly of particles. Such.
Physics 101: Lecture 12, Pg 1 Physics 101: Lecture 12 Collisions and Explosions l Today’s lecture will cover Textbook Sections Exam II.
Chapter 7 Impulse and Momentum.
UB, Phy101: Chapter 7, Pg 1 Physics 101: Chapter 7 Impulse and Momentum l Today’s lecture will cover Textbook Sections
Physics 101: Lecture 12, Pg 1 Collisions “before” “after” m1m1 m2m2 m1m1 m2m2 Explosions “before” “after” M m1m1 m2m2 Draw “before”, “after” Define system.
Linear Momentum and Collisions
Law of Conservation of Momentum. If the resultant external force on a system is zero, then the vector sum of the momentums of the objects will remain.
Collisions & Center of Mass Lecturer: Professor Stephen T. Thornton
Momentum is Conserved in an isolated system.
Physics 218: Mechanics Instructor: Dr. Tatiana Erukhimova Lecture 27.
7-6 Inelastic Collisions
Fri. Feb. 25th1 PHSX213 class Class stuff –Questions ? Conservation of Linear Momentum Collision terminology Collisions.
Section 7-4: Conservation of Energy & Momentum in Collisions
Chapter 9 Systems of Particles. Section 9.2: Center of Mass in a Two Particle System Center of Mass is the point at which all forces are assumed to act.
Copyright © 2009 Pearson Education, Inc. PHY093 Lecture 2d Linear Momentum, Impulse and Collision 1.
Conservation of Momentum & Energy in Collisions. Given some information, & using conservation laws, we can determine a LOT about collisions without knowing.
Chapter 7 Linear Momentum
About Midterm Exam 2 When and where –Thurs March 24 th 5:45-7:00 pm (after the break) –Rooms: Same as Exam I, See course webpage. –Your TA will give a.
Momentum is a Momentum vectors Impulse Defined as a Impulse is.
Momentum, Impulse, and Collisions
Physics 215 – Fall 2014Lecture Welcome back to Physics 215 Today’s agenda: More on momentum, collisions Kinetic and potential energy Potential energy.
Today: Momentum – chapter 9 11/03 Finish momentum & review for exam 11/8 Exam 2 (5 – 8) 11/10 Rotation 11/15 Gravity 11/17 Waves & Sound 11/22 Temperature.
1 PPMF102– Lecture 3 Linear Momentum. 2 Linear momentum (p) Linear momentum = mass x velocity Linear momentum = mass x velocity p = mv p = mv SI unit:
Chapter 7 Impulse and Momentum. There are many situations when the force on an object is not constant.
Chapter 7 Linear Momentum. Units of Chapter 7 Momentum and Its Relation to Force Conservation of Momentum Collisions and Impulse Conservation of Energy.
Chapter 7 Linear Momentum. MFMcGraw-PHY 1401Chap07b- Linear Momentum: Revised 6/28/ Linear Momentum Definition of Momentum Impulse Conservation.
Physics 215 – Fall 2014Lecture Welcome back to Physics 215 Today’s agenda: More gravitational potential energy Potential energy of a spring Work-kinetic.
Chapter 9 - Collisions Momentum and force Conservation of momentum
Chapter 8 Conservation of Linear Momentum Linear momentum; Momentum conservation Impulse Total kinetic energy of a system March 9, 2010.
Chapter 7 Impulse and Momentum. 7.1 The Impulse-Momentum Theorem DEFINITION OF IMPULSE The impulse of a force is the product of the average force and.
02/24/2003 Physics 103, Spring 2003, U. Wisconsin1 Physics 103: Lecture 10 Impulse and Momentum l Today’s lecture will cover the following new Concepts:
Physics 218 Lecture 15: Momentum Alexei Safonov.
System of Particles: Center-of-Mass
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 11 Momentum and Impulse l Today’s lecture will cover Textbook Sections Exam II.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 9 Physics, 4 th Edition James S. Walker.
Physics 101: Lecture 12, Pg 1 Physics 101: Lecture 12 2D Collisions and Center of mass.
Elastic and Inelastic Collisions. Elastic Collision If 2 colliding objects are very hard and no heat is produced in the collision, KE is conserved as.
Physics 101: Lecture 9, Pg 1 Physics 101: Lecture 11 Momentum and Impulse l Today’s lecture will cover Textbook Sections Exam II.
© 2007 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Chapter 8 Momentum Definition of Total Momentum The total momentum P of any number particles is equal to the vector sum of the momenta of the individual.
Your Comments I understand the concepts, but the math formulas being spat out like machine gun bullets are really confusing me. Is there a way we can see.
Physics 211 Lecture 12 Today’s Concepts: a) Elastic Collisions
Chapter 9:Linear Momentum
Lecture 12: Collisions and Explosions l Momentum Examples! è Problem Solving è Collisions (elastic & inelastic) è Explosions.
2D Collisions and Center of mass. Collisions or Explosions in Two Dimensions y x before after P total,x and P total,y independently conserved P total,x,before.
Linear Momentum Newton’s Laws of Motion First law Second law Third law.
Mechanics Lecture 11, Slide 1 Physics 211 Lecture 11 Today’s Concept: Inelastic Collisions.
Mechanics Lecture 11, Slide 1 Physics 211 Lecture 11 Today’s Concept: Momentum Conservation.
Sect. 9.2: Impulse & Momentum
Collisions: Impulse and Momentum
Momentum & Impulse Day #1: Introduction HW #7. Momentum & Collisions: Define Momentum: Momentum, p, is defined as the product of mass and velocity. Units:
Collision and Explosion
Chapter 7 Linear Momentum.
Collision and Explosion
LINEAR MOMENTUM The rate of change of the linear momentum of a particle is equal to the net force acting on the particle.
Before Class Begins Turn in homework (pgs 201 & 204) Get:
Physics 101: Lecture 12 Collisions and Explosions
Lecture Outline Chapter 9 Physics, 4th Edition James S. Walker
Homework: WS: momentum & impulse
Lecture Outline Chapter 9 Physics, 4th Edition James S. Walker
From Newton Two New Concepts Impulse & Momentum
Lecture Outline Chapter 9 Physics, 4th Edition James S. Walker
Chapter 9 : Linear Momentum
Presentation transcript:

Physics 101: Lecture 12, Pg 1 Physics 101: Lecture 12 Collisions and Explosions l Today’s lecture covers Textbook Sections Exam II

Physics 101: Lecture 12, Pg 2 Overview of Semester l Newton’s Laws   F = m a l Work-Energy   F = m a multiply both sides by d   W =  KE Energy is “conserved” è Useful when know Work done by forces l Impulse-Momentum   F = m a multiply both sides by  t   I =  p Momentum is “conserved” è Useful when EXTERNAL forces are known è Works in each direction independently

Physics 101: Lecture 12, Pg 3 Collisions “before” “after” m1m1 m2m2 m1m1 m2m2 Explosions “before” “after” M m1m1 m2m2 Draw “before”, “after” Define system so that F ext = 0 Set up axes Compute P total “before” Compute P total “after” Set them equal to each other Procedure

Physics 101: Lecture 12, Pg 4 ACT A railroad car is coasting along a horizontal track with speed V when it runs into and connects with a second identical railroad car, initially at rest. Assuming there is no friction between the cars and the rails, what is the speed of the two coupled cars after the collision? A. V B. V/2 C. V/4 D. 0 Demo with gliders  P initial =  P final M V = M V f + M V f V = 2V f V f = V/2

Physics 101: Lecture 12, Pg 5 ACT What physical quantities are conserved in the above collision? A. Only momentum is conserved B. Only total mechanical energy is conserved C. Both are conserved D. Neither are conserved CORRECT Mechanical Energy = Kinetic Energy + Potential E = ½ m v K initial = ½ m v 2 K final = ½ m (v/2) 2 + ½ m (v/2) 2 = ¼ m v 2 Elastic Collisions: collisions that conserve mechanical energy Inelastic Collisions: collisions that do not conserve mechanical energy * Completely Inelastic Collisons: objects stick together

Physics 101: Lecture 12, Pg 6 Preflight 1 & 2 Is it possible for a system of two objects to have zero total momentum and zero total kinetic energy after colliding, if both objects were moving before the collision? 1. YES 2. NO “Two cars crashing in a perfect inelastic collision.” “If two African laden swallows were flying towards each other with an equal magnitude of momentum, and they collided completely inelastically, becoming a monster two-headed African laden swallow, then the total kinetic energy after the collision is zero, and the sum of the momentums is also zero.” CORRECT Demo with gliders

Physics 101: Lecture 12, Pg 7 H LL LL m M A projectile of mass m moving horizontally with speed v strikes a stationary mass M suspended by strings of length L. Subsequently, m + M rise to a height of H. Given H, M and m what is the initial speed v of the projectile? M + m v V V=0 See I.E. 1 in homework Ballistic Pendulum demo Collision Conserves Momentum 0+m v = (M+m) V After, Conserve Energy ½ (M+m) V 2 +0 = 0+(M+m) g H V = sqrt(2 g H) Combine:

Physics 101: Lecture 12, Pg 8 Explosions “before” “after” M m1m1 m2m2 Example: m 1 = M/3 m 2 = 2M/3 Which block has larger |momentum|? * Each has same |momentum| Which block has larger speed? * mv same for each  smaller mass has larger velocity Which block has larger kinetic energy? * KE = mv 2 /2 = m 2 v 2 /2m = p 2 /2m *  smaller mass has larger KE Is mechanical (kinetic) energy conserved? * NO!! v1v1 v2v2 A=1, B=2, C=same 0 = p 1 +p 2 p 1 = -p 2

Physics 101: Lecture 12, Pg 9 Collisions or Explosions in Two Dimensions y x before after P total,x and P total,y independently conserved P total,x,before = P total,x,after P total,y,before = P total,y,after

Physics 101: Lecture 12, Pg 10 Explosions ACT “before” M A B Which of these is possible? (Ignore friction and gravity) A B C =both D = Neither “after” P x = 0 and P y = 0  P x = 0, but  P y > 0  P x = 0, and  P y = 0

Physics 101: Lecture 12, Pg 11 Center of Mass Center of Mass = Balance point l Shown is a yummy doughnut. Where would you expect the center of mass of this breakfast of champions to be located? Center of Mass! in my stomach doughnuts don't have a center of mass because they are removed and sold as doughnut hole The fact that that doughnut is "yummy" is debatable if you ask me. I prefer mine with chocolate frosting and some sort of filling. The center of mass then is much easier to figure out. It's clearly the center of the jelly or custard filling area.

Physics 101: Lecture 12, Pg 12 Center of Mass Center of Mass of a system behaves in a SIMPLE way - moves like a point particle! - velocity of CM is unaffected by collision if F ext = 0 (pork chop demo) P tot = M tot V cm F ext  t =  P tot = M tot  V cm So if F ext  = 0 then V cm is constant Also: F ext = M tot a cm

Physics 101: Lecture 12, Pg 13 Summary Collisions and Explosions Draw “before”, “after” Define system so that F ext = 0 Set up axes Compute P total “before” Compute P total “after” Set them equal to each other Center of Mass (Balance Point)